Problem 67
Question
The parametric curve given by \(x=\cos a t\) and \(y=\sin b t\) is known as a Lissajous figure. The \(x\)-coordinate oscillates \(a\) times between 1 and \(-1\) as \(t\) goes from 0 to \(2 \pi\), while the \(y\)-coordinate oscillates \(b\) times over the same \(t\) interval. This behavior is repeated over every interval of length \(2 \pi\). The entire motion takes place in a unit square. Plot the following Lissajous figures for a range of \(t\) that ensures that the resulting figure is a closed curve. In each case, count the number of times that the curve touches the horizontal and vertical borders of the unit square. (a) \(x=\sin t, y=\cos t\) (b) \(x=\sin 3 t, y=\cos 5 t\) (c) \(x=\cos 5 t, y=\sin 15 t\) (d) \(x=\sin 2 t, y=\cos 9 t\)
Step-by-Step Solution
VerifiedKey Concepts
Parametric Equations
- \(x = \cos(at)\)
- \(y = \sin(bt)\)
By adjusting \(a\) and \(b\), you can alter the complexity and shape of the figures. If the ratio of \(a:b\) is rational (i.e., both \(a\) and \(b\) can be expressed as simple fractions), the resulting curve will be closed.
Oscillation
- The \(x\)-coordinate oscillates \(a\) times between 1 and -1.
- The \(y\)-coordinate oscillates \(b\) times.
Closed Curves
For the Lissajous figures to form a closed curve, the least statistical condition is that the ratio of the frequencies \(a:b\) must be rational. This means there must be a common ratio that allows the curves to eventually reach their starting point, thus completing a loop. Without this rational ratio, the resulting figure would continue indefinitely without closure.
The process of calculating the exact range of \(t\) needed for closure involves finding a period where the components of the curve - each described by the trigonometric functions - successfully synchronize to return to the beginning. Usually, this is understood by computing the least common multiple (LCM) of their periods.
Least Common Multiple
To determine the appropriate range of \(t\) for closure, calculate the LCM of the periods of the oscillations defined by \(2\pi/a\) and \(2\pi/b\). This computes the smallest value of \(t\) that satisfies both oscillation cycles simultaneously. For example, in cases where \(t\) extends from 0 to \(2\pi\), as in the exercise scenarios, the LCM helps to ascertain that the figure indeed closes after completing the requisite number of oscillations.
This mathematical analysis ensures that the Lissajous figure appears complete and coherent, resulting in the striking symmetrical patterns known to capture observers' imaginations.